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Integrable and Conformal Boundary Conditions for $widehat{sell}$ (2) A–D–E Lattice Models and Unitary Minimal Conformal Field Theories

机译:$ widehat {sell} $(2)A–D–E格模型和Unit最小保形场理论的可积和共形边界条件

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摘要

Integrable boundary conditions are studied for critical A–D–E and general graph-based lattice models of statistical mechanics. In particular, using techniques associated with the Temperley–Lieb algebra and fusion, a set of boundary Boltzmann weights which satisfies the boundary Yang–Baxter equation is obtained for each boundary condition. When appropriately specialized, these boundary weights, each of which depends on three spins, decompose into more natural two-spin edge weights. The specialized boundary conditions for the A–D–E cases are naturally in one-to-one correspondence with the conformal boundary conditions of $widehat{sell }$ (2) unitary minimal conformal field theories. Supported by this and further evidence, we conclude that, in the continuum scaling limit, the integrable boundary conditions provide realizations of the complete set of conformal boundary conditions in the corresponding field theories.
机译:研究了临界A–D–E和基于统计力学的基于一般图的网格模型的可积边界条件。特别是,使用与Temperley-Lieb代数和融合相关的技术,可以为每个边界条件获得一组满足边界Yang-Baxter方程的边界Boltzmann权重。如果适当地进行了专门化,则这些边界权重(分别取决于三个自旋)将分解为更自然的两个自旋边缘权重。 A–D–E情况的特殊边界条件自然与$ widehat {sell} $(2)minimal最小共形共形场理论的共形边界条件一一对应。在此证据和进一步的证据支持下,我们得出结论,在连续标度极限内,可积分边界条件提供了相应场论中完整的共形边界条件集的实现。

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